[en] We revisit the problem of Q-colourings of the triangular lattice using a mapping onto an integrable spin-one model, which can be solved exactly using Bethe ansatz techniques. In particular we focus on the low-energy excitations above the eigenlevel g ₂, which was shown by Baxter to dominate the transfer matrix spectrum in the Fortuin–Kasteleyn (chromatic polynomial) representation for $Q_0⩽<!--\; ???\; -->Q⩽<!--\; ???\; -->4$, where $Q_0=3.819671\cdots <!--\; ???\; -->$. We argue that g ₂ and its scaling levels define a conformally invariant theory, the so-called regime IV, which provides the actual description of the (analytically continued) colouring problem within a much wider range, namely $Q\in <!--\; ???\; -->(2,4]$. The corresponding conformal field theory is identified and the exact critical exponents are derived. We discuss their implications for the phase diagram of the antiferromagnetic triangular-lattice Potts model at non-zero temperature. Finally, we relate our results to recent observations in the field of spin-one anyonic chains. (paper)